JPH0191680A - Motor - Google Patents
MotorInfo
- Publication number
- JPH0191680A JPH0191680A JP24645587A JP24645587A JPH0191680A JP H0191680 A JPH0191680 A JP H0191680A JP 24645587 A JP24645587 A JP 24645587A JP 24645587 A JP24645587 A JP 24645587A JP H0191680 A JPH0191680 A JP H0191680A
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- JP
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- Prior art keywords
- current
- elements
- magnet
- poles
- superconducting
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000004020 conductor Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
Landscapes
- Superconductive Dynamoelectric Machines (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、マグネットと超電導素子で形成される電動機
に関する。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to an electric motor formed of a magnet and a superconducting element.
従来の技術
従来、電動機はマグネットとコイルで構成されており、
コイルに電流を流すことによフトルクが発生し、それに
よって電動機が回転する。Conventional technology Traditionally, electric motors are composed of magnets and coils.
By passing current through the coil, torque is generated, which causes the motor to rotate.
発明が解決しようとする問題点
このような従来の構成において、電動機を回転させるに
はコイルに電流を流す必要があり、低消費電流を実現す
ることが困難である。Problems to be Solved by the Invention In such a conventional configuration, it is necessary to pass current through the coil in order to rotate the motor, and it is difficult to achieve low current consumption.
本発明は、上記問題点を解決することを目的とし、少な
い電流で回転可能な電動機を提供することを目的とする
。The present invention aims to solve the above-mentioned problems, and aims to provide an electric motor that can rotate with a small amount of current.
問題点を解決するための手段
本発明は、着磁極数にの固定マグネットと、着磁極数乙
の回転マグネットを対向して配し0.複数個の超電導素
子から成る磁場切換体を固定マグネットと回転マグネッ
トの間に配するように構成され、前記回転マグネットの
回転位置に対応して前記超電導素子の少なくとも1つを
超電導状態あるいは常電導状態に切9換えることを特徴
とする電動機である。Means for Solving the Problems In the present invention, a fixed magnet with a number of magnetized poles and a rotating magnet with a number of magnetized poles are arranged facing each other. A magnetic field switching body composed of a plurality of superconducting elements is arranged between a fixed magnet and a rotating magnet, and at least one of the superconducting elements is switched to a superconducting state or a normal conducting state in accordance with the rotational position of the rotating magnet. This electric motor is characterized by being able to switch between 9 and 9 times.
作用
本発明は上記した構成により、超電導素子を常電導状態
とする時にのみ、超電導素子に微小電流を流すことで電
動機を回転することができ、低消費電流の電動機を実現
することができる。According to the present invention, with the above-described configuration, the motor can be rotated by passing a minute current through the superconducting element only when the superconducting element is in a normal conducting state, and a motor with low current consumption can be realized.
実施例
第1図に本発明における一実施例の電動機を構成する部
材を示す。第1図aは8極に着磁された固定マグネット
1を示す。同図すは8個の超電導素子6a〜6dを有し
て成る磁場切換体2を示す。Embodiment FIG. 1 shows members constituting an electric motor according to an embodiment of the present invention. FIG. 1a shows a fixed magnet 1 magnetized into eight poles. The figure shows a magnetic field switching body 2 comprising eight superconducting elements 6a to 6d.
同図Cは12極に着磁された回転マグネットを示す。Figure C shows a rotating magnet magnetized to 12 poles.
固定マグネット1、磁場切換体2、回転マグネット3は
第2図aに示すように配される。すなわち固定マグネッ
ト1、磁場切換体2、回転マグネット3の順で、それぞ
れが対向するように配される。The fixed magnet 1, the magnetic field switching body 2, and the rotating magnet 3 are arranged as shown in FIG. 2a. That is, the fixed magnet 1, the magnetic field switching body 2, and the rotating magnet 3 are arranged in this order so as to face each other.
また超電導素子5&、50は固定マグネット1のS極に
対向し、かつ超電導素子5b、5dは固定マグネット1
のN極に対向するように配されている。磁場切換体2は
超電導部材4と超電導素子6a〜6dで成る。超電導素
子6a〜6dは通常超電導特性を有しておシ、磁界を通
さない(マイスナー効果)。一方臨界電流Ia以上の電
流を流すと超電導素子5a〜6dは超電導特性を失ない
、常電導となり磁界を通す。Further, the superconducting elements 5&, 50 are opposed to the S pole of the fixed magnet 1, and the superconducting elements 5b, 5d are opposite to the S pole of the fixed magnet 1.
It is arranged so as to face the N pole of. The magnetic field switching body 2 consists of a superconducting member 4 and superconducting elements 6a to 6d. The superconducting elements 6a to 6d usually have superconducting properties and do not allow magnetic fields to pass through them (Meissner effect). On the other hand, when a current higher than the critical current Ia is applied, the superconducting elements 5a to 6d do not lose their superconducting properties, but become normal conductors and pass a magnetic field.
この特性を利用して回転マグネットを回転させる動作を
第2図を用いて説明する。前述したように、固定マグネ
ット1と回転マグネット3が対向して配され、かつ固定
マグネット1と回転マグネット3の間には磁場切換体2
が配されている。超電導素子6a〜6dは回転マグネッ
ト3の回転位置に対応して通電が切シ換えられる。まず
超電導素子6aに臨界電流I&以上の電流を流し、常電
導とすると、固定マグネット1のS極と回転マグネット
3のN極が引き合い、よって第2図aに示すような位置
関係となる。次に超電導素子6aへの通電を中止し、超
電導素子6bに臨界電流Ia以上の電流を流すと、超電
導素子6bは常電導となり、よって回転マグネット3の
回転位置は第2図すに示すようになる。次に超電導素子
5b−\の通電を中止し、超電導素子6oに臨界電流工
&以上の電流を流すと、超電導素子6cは常電導となシ
、よって回転マグネット3の回転位置は第2図Cに示す
ようになる。次に超電導素子6cへの通電を中止し、超
電導素子6dに臨界電流Ia以上の電流を流すと、超電
導素子6dは常電導となシ、よって回転マグネット3の
回転位置は第2図dに示すようになる。The operation of rotating the rotating magnet using this characteristic will be explained using FIG. 2. As mentioned above, the fixed magnet 1 and the rotating magnet 3 are arranged facing each other, and the magnetic field switching body 2 is provided between the fixed magnet 1 and the rotating magnet 3.
are arranged. The superconducting elements 6a to 6d are energized depending on the rotational position of the rotating magnet 3. First, when a current equal to or higher than the critical current I& is applied to the superconducting element 6a to make it normal conductive, the S pole of the fixed magnet 1 and the N pole of the rotating magnet 3 attract each other, resulting in a positional relationship as shown in FIG. 2a. Next, when the power supply to the superconducting element 6a is stopped and a current higher than the critical current Ia is applied to the superconducting element 6b, the superconducting element 6b becomes normal conductive, and therefore the rotational position of the rotating magnet 3 is changed as shown in FIG. Become. Next, when the superconducting element 5b-\ is de-energized and a current equal to or higher than the critical current is passed through the superconducting element 6o, the superconducting element 6c becomes normal conductive, and therefore the rotational position of the rotating magnet 3 is set to C in Fig. 2. It becomes as shown in . Next, when the power supply to the superconducting element 6c is stopped and a current equal to or higher than the critical current Ia is passed through the superconducting element 6d, the superconducting element 6d becomes normal conductive, and therefore, the rotational position of the rotating magnet 3 is shown in FIG. 2d. It becomes like this.
以上説明したように、回転マグネット3の回転位置に対
応して、超電導素子6&〜6dへの通電を切シ換え、超
電導状態と常電導状態を切り換えることで、回転マグネ
ット3を回転させることができる。As explained above, the rotating magnet 3 can be rotated by switching the energization to the superconducting elements 6 & ~ 6d and switching between the superconducting state and the normal conducting state in accordance with the rotational position of the rotating magnet 3. .
この時に回転マグネット3を回転させるのに必要な電流
は臨界電流Ia以上であればよく、数μÅ以下の微小な
電流で回転させることができる。At this time, the current required to rotate the rotating magnet 3 may be greater than or equal to the critical current Ia, and rotation can be achieved with a minute current of several microangstroms or less.
発明の詳細
な説明したように、本発明によれば微小な消費電流で電
動機の回転を実現することができるという効果がある。As described in detail, the present invention has the advantage that it is possible to realize the rotation of the electric motor with a small amount of current consumption.
第1図は本発明における一実施例の電動機を構成する部
材の平面図、第2図は本発明の電動機の動作を説明する
ための補助図である。
1・・・・・・固定マグネット、2・・・・・・磁場切
換体、3・・・・・・回転マグネット、5J 5b、5
0,5d ・・川・超電導素子。FIG. 1 is a plan view of members constituting an electric motor according to an embodiment of the present invention, and FIG. 2 is an auxiliary diagram for explaining the operation of the electric motor according to the present invention. 1... Fixed magnet, 2... Magnetic field switching body, 3... Rotating magnet, 5J 5b, 5
0,5d... River superconducting element.
Claims (2)
マグネットを対向して配し、複数個の超電導素子から成
る磁場切換体を前記固定マグネットと回転マグネットの
間に配するように構成され、前記回転マグネットの回転
位置に対応して前記超電導素子の少なくとも1つを超電
導状態あるいは常電導状態に切り換えることを特徴とす
る電動機。(1) A fixed magnet with a number of magnetized poles K and a rotating magnet with a number of magnetized poles L are arranged to face each other, and a magnetic field switching body made of a plurality of superconducting elements is arranged between the fixed magnet and the rotating magnet. An electric motor characterized in that at least one of the superconducting elements is switched to a superconducting state or a normal conducting state in accordance with the rotational position of the rotating magnet.
着磁極数Lの関係は(K:L)=(2:3)となること
を特徴とする特許請求の範囲第1項記載の電動機。(2) The electric motor according to claim 1, wherein the relationship between the number K of magnetized poles of the fixed magnet and the number L of magnetized poles of the rotating magnet is (K:L)=(2:3).
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24645587A JPH0191680A (en) | 1987-09-30 | 1987-09-30 | Motor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP24645587A JPH0191680A (en) | 1987-09-30 | 1987-09-30 | Motor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0191680A true JPH0191680A (en) | 1989-04-11 |
Family
ID=17148685
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP24645587A Pending JPH0191680A (en) | 1987-09-30 | 1987-09-30 | Motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0191680A (en) |
-
1987
- 1987-09-30 JP JP24645587A patent/JPH0191680A/en active Pending
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